Manipulation of the domain wall propagation in magnetic wires is a key practical task for a number of devices including racetrack memory and magnetic logic. Recently, curvilinear effects emerged as an efficient mean to impact substantially the statics and dynamics of magnetic textures. Here, we demonstrate that the curvilinear form of the exchange interaction of a magnetic helix results in an effective anisotropy term and Dzyaloshinskii-Moriya interaction with a complete set of Lifshitz invariants for a one-dimensional system. In contrast to their planar counterparts, the geometrically induced modifications of the static magnetic texture of the domain walls in magnetic helices offer unconventional means to control the wall dynamics relying on spin-orbit Rashba torque. The chiral symmetry breaking due to the Dzyaloshinskii-Moriya interaction leads to the opposite directions of the domain wall motion in left-or right-handed helices. Furthermore, for the magnetic helices, the emergent effective anisotropy term and Dzyaloshinskii-Moriya interaction can be attributed to the clear geometrical parameters like curvature and torsion offering intuitive understanding of the complex curvilinear effects in magnetism.
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South China Normal Univ, Inst Adv Mat, South China Acad Adv Optoelect, Guangzhou 510006, Guangdong, Peoples R China
South China Normal Univ, Guangdong Prov Key Lab Quantum Engn & Quantum Mat, Guangzhou 510006, Guangdong, Peoples R ChinaSouth China Normal Univ, Inst Adv Mat, South China Acad Adv Optoelect, Guangzhou 510006, Guangdong, Peoples R China
Yan, Zhengren
Chen, Zhiyuan
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South China Normal Univ, Inst Adv Mat, South China Acad Adv Optoelect, Guangzhou 510006, Guangdong, Peoples R China
South China Normal Univ, Guangdong Prov Key Lab Quantum Engn & Quantum Mat, Guangzhou 510006, Guangdong, Peoples R ChinaSouth China Normal Univ, Inst Adv Mat, South China Acad Adv Optoelect, Guangzhou 510006, Guangdong, Peoples R China
Chen, Zhiyuan
Qin, Minghui
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South China Normal Univ, Inst Adv Mat, South China Acad Adv Optoelect, Guangzhou 510006, Guangdong, Peoples R China
South China Normal Univ, Guangdong Prov Key Lab Quantum Engn & Quantum Mat, Guangzhou 510006, Guangdong, Peoples R ChinaSouth China Normal Univ, Inst Adv Mat, South China Acad Adv Optoelect, Guangzhou 510006, Guangdong, Peoples R China
Qin, Minghui
Lu, Xubing
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South China Normal Univ, Inst Adv Mat, South China Acad Adv Optoelect, Guangzhou 510006, Guangdong, Peoples R China
South China Normal Univ, Guangdong Prov Key Lab Quantum Engn & Quantum Mat, Guangzhou 510006, Guangdong, Peoples R ChinaSouth China Normal Univ, Inst Adv Mat, South China Acad Adv Optoelect, Guangzhou 510006, Guangdong, Peoples R China
Lu, Xubing
Gao, Xingsen
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South China Normal Univ, Inst Adv Mat, South China Acad Adv Optoelect, Guangzhou 510006, Guangdong, Peoples R China
South China Normal Univ, Guangdong Prov Key Lab Quantum Engn & Quantum Mat, Guangzhou 510006, Guangdong, Peoples R ChinaSouth China Normal Univ, Inst Adv Mat, South China Acad Adv Optoelect, Guangzhou 510006, Guangdong, Peoples R China
Gao, Xingsen
Liu, Junming
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Nanjing Univ, Lab Solid State Microstruct, Nanjing 210093, Jiangsu, Peoples R China
Nanjing Univ, Innovat Ctr Adv Microstruct, Nanjing 210093, Jiangsu, Peoples R ChinaSouth China Normal Univ, Inst Adv Mat, South China Acad Adv Optoelect, Guangzhou 510006, Guangdong, Peoples R China
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Rzeszow Univ Technol, Dept Phys & Med Engn, Al Powstancow Warszawy 6, PL-35959 Rzeszow, PolandRzeszow Univ Technol, Dept Phys & Med Engn, Al Powstancow Warszawy 6, PL-35959 Rzeszow, Poland
Inglot, M.
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Barnas, J.
Dugaev, V. K.
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Rzeszow Univ Technol, Dept Phys & Med Engn, Al Powstancow Warszawy 6, PL-35959 Rzeszow, PolandRzeszow Univ Technol, Dept Phys & Med Engn, Al Powstancow Warszawy 6, PL-35959 Rzeszow, Poland